2015
DOI: 10.1093/mnras/stv1047
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The orbital evolution of asteroids, pebbles and planets from giant branch stellar radiation and winds

Abstract: The discovery of over 50 planets around evolved stars and more than 35 debris discs orbiting white dwarfs highlight the increasing need to understand small body evolution around both early and asymptotic giant branch (GB) stars. Pebbles and asteroids are susceptible to strong accelerations from the intense luminosity and winds of GB stars. Here, we establish equations that can model time-varying GB stellar radiation, wind drag and mass loss. We derive the complete three-dimensional equations of motion in orbit… Show more

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Cited by 65 publications
(107 citation statements)
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References 123 publications
(143 reference statements)
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“…The asteroid further would be too large to be circularized by radiation alone, either through the Yarkovsky effect or Poynting-Robertson drag (Veras et al 2015a(Veras et al , 2015c. One possibility is that some fraction of the asteroid has sublimated.…”
Section: Discussionmentioning
confidence: 99%
“…The asteroid further would be too large to be circularized by radiation alone, either through the Yarkovsky effect or Poynting-Robertson drag (Veras et al 2015a(Veras et al , 2015c. One possibility is that some fraction of the asteroid has sublimated.…”
Section: Discussionmentioning
confidence: 99%
“…In this case, the exomoon would become an exoring, and this exoring would be subject to a similar type of disruption from close encounters with other planets during gravitational scattering on the WD phase. If the moon survives spin-up, then GB radiation could alter its orbit (Veras, Eggl & Gänsicke 2015a), potentially allowing it to drift closer to the edge of the planet's Hill radius. Just how the orbital parameters of the moon would be affected by this radiation is non-trivial and requires future exploration.…”
Section: Additional Considerationsmentioning
confidence: 99%
“…2 of Mustill et al 2014). By adopting this mass-loss rate, we can derive max(ρ wind ) by assuming a spherically symmetric wind and using equation (5) from Dong et al (2010) or equation (54) from Veras et al (2015a). Consequently, we find max(ρ wind ) = max(Ṁ )/(4πa 2 P v wind ) = 3.1 × 10 −45 ap 30 au −2 M m −3 , assuming that v wind corresponds to the escape speed from a typical WD (4 × 10 3 km s −1 ).…”
Section: A P P E N D I X B : E N C L O S E D M a S S W I T H I N M O mentioning
confidence: 99%
“…It must also be mentioned that other mechanisms, some of which not yet well understood, could also produce the observed excitation of the MB. One example is the recent work by Veras et al (2015), which models the orbital evolution of asteroids under the effect of stellar radiation and winds. In particular, the authors study the long-lasting Yarkovsky effects on the eccentricity and inclination evolution of the small bodies.…”
Section: Dynamical Excitationmentioning
confidence: 99%